ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY GUIDED BY Prof. R.H.Chaudhary Prof. R.H.Chaudhary Asst.prof in electrical Asst.prof in electrical Department Department PREPARED BY PREPARED BY Rajpurohit Anurag ( ) Rajpurohit Anurag ( ) Soneri Sahil ( ) Soneri Sahil ( ) Vaghasiya Chirag ( ) Vaghasiya Chirag ( ) Bhati Sejal ( ) Bhati Sejal ( )

An AC circuit consists of a combination of circuit elements and an AC generator or source An AC circuit consists of a combination of circuit elements and an AC generator or source The output of an AC generator is sinusoidal and varies with time according to the following equation The output of an AC generator is sinusoidal and varies with time according to the following equation Δv = ΔV max sin 2  ƒt Δv = ΔV max sin 2  ƒt Δv is the instantaneous voltage Δv is the instantaneous voltage ΔV max is the maximum voltage of the generator ΔV max is the maximum voltage of the generator ƒ is the frequency at which the voltage changes, in Hz ƒ is the frequency at which the voltage changes, in Hz AC Circuit

Resistor in an AC Circuit Consider a circuit consisting of an AC source and a resistor Consider a circuit consisting of an AC source and a resistor The graph shows the current through and the voltage across the resistor The graph shows the current through and the voltage across the resistor The current and the voltage reach their maximum values at the same time The current and the voltage reach their maximum values at the same time The current and the voltage are said to be in phase The current and the voltage are said to be in phase

More About Resistors in an AC Circuit The direction of the current has no effect on the behavior of the resistor The direction of the current has no effect on the behavior of the resistor The rate at which electrical energy is dissipated in the circuit is given by The rate at which electrical energy is dissipated in the circuit is given by P = i 2 R P = i 2 R where i is the instantaneous current where i is the instantaneous current the heating effect produced by an AC current with a maximum value of I max is not the same as that of a DC current of the same value the heating effect produced by an AC current with a maximum value of I max is not the same as that of a DC current of the same value The maximum current occurs for a small amount of time The maximum current occurs for a small amount of time

rms Current and Voltage The rms current is the direct current that would dissipate the same amount of energy in a resistor as is actually dissipated by the AC current The rms current is the direct current that would dissipate the same amount of energy in a resistor as is actually dissipated by the AC current Alternating voltages can also be discussed in terms of rms values Alternating voltages can also be discussed in terms of rms values

Ohm’s Law in an AC Circuit rms values will be used when discussing AC currents and voltages rms values will be used when discussing AC currents and voltages AC ammeters and voltmeters are designed to read rms values AC ammeters and voltmeters are designed to read rms values Many of the equations will be in the same form as in DC circuits Many of the equations will be in the same form as in DC circuits Ohm’s Law for a resistor, R, in an AC circuit Ohm’s Law for a resistor, R, in an AC circuit ΔV rms = I rms R ΔV rms = I rms R Also applies to the maximum values of v and i Also applies to the maximum values of v and i

Capacitors in an AC Circuit Consider a circuit containing a capacitor and an AC source Consider a circuit containing a capacitor and an AC source The current starts out at a large value and charges the plates of the capacitor The current starts out at a large value and charges the plates of the capacitor There is initially no resistance to hinder the flow of the current while the plates are not charged There is initially no resistance to hinder the flow of the current while the plates are not charged As the charge on the plates increases, the voltage across the plates increases and the current flowing in the circuit decreases As the charge on the plates increases, the voltage across the plates increases and the current flowing in the circuit decreases

More About Capacitors in an AC Circuit The current reverses direction The current reverses direction The voltage across the plates decreases as the plates lose the charge they had accumulated The voltage across the plates decreases as the plates lose the charge they had accumulated The voltage across the capacitor lags behind the current by 90° The voltage across the capacitor lags behind the current by 90°

Capacitive Reactance and Ohm’s Law The impeding effect of a capacitor on the current in an AC circuit is called the capacitive reactance and is given by The impeding effect of a capacitor on the current in an AC circuit is called the capacitive reactance and is given by When ƒ is in Hz and C is in F, X C will be in ohms When ƒ is in Hz and C is in F, X C will be in ohms Ohm’s Law for a capacitor in an AC circuit Ohm’s Law for a capacitor in an AC circuit ΔV rms = I rms X C ΔV rms = I rms X C

Inductors in an AC Circuit Consider an AC circuit with a source and an inductor Consider an AC circuit with a source and an inductor The current in the circuit is impeded by the back emf of the inductor The current in the circuit is impeded by the back emf of the inductor The voltage across the inductor always leads the current by 90° The voltage across the inductor always leads the current by 90°

Inductive Reactance and Ohm’s Law The effective resistance of a coil in an AC circuit is called its inductive reactance and is given by The effective resistance of a coil in an AC circuit is called its inductive reactance and is given by X L = 2  ƒL X L = 2  ƒL When ƒ is in Hz and L is in H, X L will be in ohms When ƒ is in Hz and L is in H, X L will be in ohms Ohm’s Law for the inductor Ohm’s Law for the inductor ΔV rms = I rms X L ΔV rms = I rms X L

The RLC Series Circuit The resistor, inductor, and capacitor can be combined in a circuit The resistor, inductor, and capacitor can be combined in a circuit The current in the circuit is the same at any time and varies sinusoidally with time The current in the circuit is the same at any time and varies sinusoidally with time

Current and Voltage Relationships in an RLC Circuit The instantaneous voltage across the resistor is in phase with the current The instantaneous voltage across the resistor is in phase with the current The instantaneous voltage across the inductor leads the current by 90° The instantaneous voltage across the inductor leads the current by 90° The instantaneous voltage across the capacitor lags the current by 90° The instantaneous voltage across the capacitor lags the current by 90°

Phasor Diagrams To account for the different phases of the voltage drops, vector techniques are used To account for the different phases of the voltage drops, vector techniques are used Represent the voltage across each element as a rotating vector, called a phasor Represent the voltage across each element as a rotating vector, called a phasor The diagram is called a phasor diagram The diagram is called a phasor diagram

Phasor Diagram for RLC Series Circuit The voltage across the resistor is on the +x axis since it is in phase with the current The voltage across the resistor is on the +x axis since it is in phase with the current The voltage across the inductor is on the +y since it leads the current by 90° The voltage across the inductor is on the +y since it leads the current by 90° The voltage across the capacitor is on the –y axis since it lags behind the current by 90° The voltage across the capacitor is on the –y axis since it lags behind the current by 90°

Phasor Diagram, cont The phasors are added as vectors to account for the phase differences in the voltages The phasors are added as vectors to account for the phase differences in the voltages ΔV L and ΔV C are on the same line and so the net y component is ΔV L - ΔV C ΔV L and ΔV C are on the same line and so the net y component is ΔV L - ΔV C

ΔV max From the Phasor Diagram The voltages are not in phase, so they cannot simply be added to get the voltage across the combination of the elements or the voltage source The voltages are not in phase, so they cannot simply be added to get the voltage across the combination of the elements or the voltage source  is the phase angle between the current and the maximum voltage  is the phase angle between the current and the maximum voltage

Impedance of a Circuit The impedance, Z, can also be represented in a phasor diagram The impedance, Z, can also be represented in a phasor diagram

Impedance and Ohm’s Law Ohm’s Law can be applied to the impedance Ohm’s Law can be applied to the impedance ΔV max = I max Z ΔV max = I max Z

Summary of Circuit Elements, Impedance and Phase Angles

Problem Solving for AC Circuits Calculate as many unknown quantities as possible Calculate as many unknown quantities as possible For example, find X L and X C For example, find X L and X C Be careful of units -- use F, H, Ω Be careful of units -- use F, H, Ω Apply Ohm’s Law to the portion of the circuit that is of interest Apply Ohm’s Law to the portion of the circuit that is of interest Determine all the unknowns asked for in the problem Determine all the unknowns asked for in the problem

Power in an AC Circuit, cont The average power delivered by the generator is converted to internal energy in the resistor The average power delivered by the generator is converted to internal energy in the resistor P av = I rms ΔV R = I rms ΔV rms cos  P av = I rms ΔV R = I rms ΔV rms cos  cos  is called the power factor of the circuit cos  is called the power factor of the circuit Phase shifts can be used to maximize power outputs Phase shifts can be used to maximize power outputs

Maxwell’s Starting Points Electric field lines originate on positive charges and terminate on negative charges Electric field lines originate on positive charges and terminate on negative charges Magnetic field lines always form closed loops – they do not begin or end anywhere Magnetic field lines always form closed loops – they do not begin or end anywhere A varying magnetic field induces an emf and hence an electric field (Faraday’s Law) A varying magnetic field induces an emf and hence an electric field (Faraday’s Law) Magnetic fields are generated by moving charges or currents (Ampère’s Law) Magnetic fields are generated by moving charges or currents (Ampère’s Law)

Hertz’s Basic LC Circuit When the switch is closed, oscillations occur in the current and in the charge on the capacitor When the switch is closed, oscillations occur in the current and in the charge on the capacitor When the capacitor is fully charged, the total energy of the circuit is stored in the electric field of the capacitor When the capacitor is fully charged, the total energy of the circuit is stored in the electric field of the capacitor At this time, the current is zero and no energy is stored in the inductor At this time, the current is zero and no energy is stored in the inductor

LC Circuit, cont As the capacitor discharges, the energy stored in the electric field decreases As the capacitor discharges, the energy stored in the electric field decreases At the same time, the current increases and the energy stored in the magnetic field increases At the same time, the current increases and the energy stored in the magnetic field increases When the capacitor is fully discharged, there is no energy stored in its electric field When the capacitor is fully discharged, there is no energy stored in its electric field The current is at a maximum and all the energy is stored in the magnetic field in the inductor The current is at a maximum and all the energy is stored in the magnetic field in the inductor The process repeats in the opposite direction The process repeats in the opposite direction There is a continuous transfer of energy between the inductor and the capacitor There is a continuous transfer of energy between the inductor and the capacitor

Electromagnetic Waves are Transverse Waves The E and B fields are perpendicular to each other The E and B fields are perpendicular to each other Both fields are perpendicular to the direction of motion Both fields are perpendicular to the direction of motion Therefore, em waves are transverse waves Therefore, em waves are transverse waves